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Faraday instability on a sphere: numerical simulation

Published online by Cambridge University Press:  10 May 2019

A. Ebo-Adou
Affiliation:
Physique et Mécanique des Milieux Hétérogènes (PMMH), CNRS, ESPCI Paris, PSL Research University, Sorbonne Université, Univ. Paris Diderot, 75005, France Laboratoire d’Informatique pour la Mécanique et les Sciences de l’Ingénieur (LIMSI), Centre National de la Recherche Scientifique (CNRS), Université Paris Saclay, Bât. 507, Rue du Belvédère, Campus Universitaire, 91405 Orsay, France Institut des Sciences de la Terre, Centre d’Études et de Recherche de Djibouti, Route de l’aéroport B.P 486 Djibouti-ville, République de Djibouti
L. S. Tuckerman*
Affiliation:
Physique et Mécanique des Milieux Hétérogènes (PMMH), CNRS, ESPCI Paris, PSL Research University, Sorbonne Université, Univ. Paris Diderot, 75005, France
S. Shin
Affiliation:
Department of Mechanical and System Design Engineering, Hongik University, Seoul 121-791, Republic of Korea
J. Chergui
Affiliation:
Laboratoire d’Informatique pour la Mécanique et les Sciences de l’Ingénieur (LIMSI), Centre National de la Recherche Scientifique (CNRS), Université Paris Saclay, Bât. 507, Rue du Belvédère, Campus Universitaire, 91405 Orsay, France
D. Juric
Affiliation:
Laboratoire d’Informatique pour la Mécanique et les Sciences de l’Ingénieur (LIMSI), Centre National de la Recherche Scientifique (CNRS), Université Paris Saclay, Bât. 507, Rue du Belvédère, Campus Universitaire, 91405 Orsay, France
*
Email address for correspondence: laurette@pmmh.espci.fr

Abstract

We consider a spherical variant of the Faraday problem, in which a spherical drop is subjected to a time-periodic body force, as well as surface tension. We use a full three-dimensional parallel front-tracking code to calculate the interface motion of the parametrically forced oscillating viscous drop, as well as the velocity field inside and outside the drop. Forcing frequencies are chosen so as to excite spherical harmonic wavenumbers ranging from 1 to 6. We excite gravity waves for wavenumbers 1 and 2 and observe translational and oblate–prolate oscillation, respectively. For wavenumbers 3 to 6, we excite capillary waves and observe patterns analogous to the Platonic solids. For low viscosity, both subharmonic and harmonic responses are accessible. The patterns arising in each case are interpreted in the context of the theory of pattern formation with spherical symmetry.

Type
JFM Papers
Copyright
© 2019 Cambridge University Press 

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References

Arbell, H. & Fineberg, J. 2002 Pattern formation in two-frequency forced parametric waves. Phys. Rev. E 65, 036224.Google ScholarPubMed
Basaran, O. A. 1992 Nonlinear oscillations of viscous liquid drops. J. Fluid Mech. 241, 169198.CrossRefGoogle Scholar
Busse, F. H. 1975 Patterns of convection in spherical shells. J. Fluid Mech. 72, 6785.CrossRefGoogle Scholar
Busse, F. H. & Riahi, N. 1982 Patterns of convection in spherical shells. Part 2. J. Fluid Mech. 123, 283301.CrossRefGoogle Scholar
Chorin, A. J. 1968 Numerical simulation of the Navier–Stokes equations. Math. Comput. 22, 745762.CrossRefGoogle Scholar
Chossat, P., Lauterbach, R. & Melbourne, I. 1991 Steady-state bifurcation with O (3) symmetry. Arch. Rat. Mech. Anal. 113, 313376.CrossRefGoogle Scholar
Douady, S. 1990 Experimental study of the Faraday instability. J. Fluid Mech. 221, 383409.CrossRefGoogle Scholar
Ebo-Adou, A. & Tuckerman, L. S. 2016 Faraday instability on a sphere: Floquet analysis. J. Fluid Mech. 805, 591610.CrossRefGoogle Scholar
Edwards, W. S. & Fauve, S. 1994 Patterns and quasi-patterns in the Faraday experiment. J. Fluid Mech. 278, 123148.CrossRefGoogle Scholar
Faraday, M. 1831 On a peculiar class of acoustical figures; and on certain forms assumed by groups of particles upon vibrating elastic surfaces. Phil. Trans. R. Soc. Lond. A 121, 299340.Google Scholar
Golubitsky, M., Stewart, I. & Schaeffer, D. G. 1988 Singularities and Groups in Bifurcation Theory: Vol. II. Springer.CrossRefGoogle Scholar
Harlow, F. H. & Welch, J. E. 1965 Numerical calculation of time dependent viscous incompressible flow of fluid with free surface. Phys. Fluids 8, 2182.CrossRefGoogle Scholar
Ihrig, E. & Golubitsky, M. 1984 Pattern selection with O (3) symmetry. Physica D 13, 133.Google Scholar
Kahouadji, L., Périnet, N., Tuckerman, L. S., Shin, S., Chergui, J. & Juric, D. 2015 Numerical simulation of supersquare patterns in Faraday waves. J. Fluid Mech. 772, R2.CrossRefGoogle Scholar
Kudrolli, A., Pier, B. & Gollub, J. P. 1998 Superlattice patterns in surface waves. Physica D 123, 99111.Google Scholar
Kumar, K. 1996 Linear theory of Faraday instability in viscous fluids. Proc. R. Soc. Lond. 452, 11131126.Google Scholar
Kumar, K. & Tuckerman, L. S. 1994 Parametric instability of the interface between two fluids. J. Fluid Mech. 279, 4968.CrossRefGoogle Scholar
Kwak, D. Y. & Lee, J. S. 2004 Multigrid algorithm for the cell-centered finite-difference method II: discontinuous coefficient case. Numer. Methods Partial Differential Equations 20, 723741.CrossRefGoogle Scholar
Lamb, H. 1932 Hydrodynamics. Cambridge University Press.Google Scholar
Lundgren, T. S. & Mansour, N. N. 1988 Oscillations of drops in zero gravity with weak viscous effects. J. Fluid Mech. 194, 479510.CrossRefGoogle Scholar
Matthews, P. C. 2003 Pattern formation on a sphere. Phys. Rev. E 67, 036206.Google Scholar
Meradji, S., Lyubimova, T. P., Lyubimov, D. V. & Roux, B. 2001 Numerical simulation of a liquid drop freely oscillating. Cryst. Res. Technol. 36, 729744.3.0.CO;2-3>CrossRefGoogle Scholar
Patzek, T., Benner, R., Basaran, O. & Scriven, L. 1991 Nonlinear oscillations of inviscid free drops. J. Comput. Phys. 97, 489515.CrossRefGoogle Scholar
Périnet, N., Juric, D. & Tuckerman, L. S. 2012 Alternating hexagonal and striped patterns in Faraday surface waves. Phys. Rev. Lett. 109, 164501.CrossRefGoogle ScholarPubMed
Peskin, C. S. 1977 Numerical analysis of blood flow in the heart. J. Comput. Phys. 25, 220252.CrossRefGoogle Scholar
Politis, A.2016 Microphone array processing for parametric spatial audio techniques. PhD thesis, Aalto University, Finland.Google Scholar
Popinet, S. 1993 Gerris: a tree-based adaptive solver for the incompressible Euler equations in complex geometries. J. Comput. Phys. 190, 572600.CrossRefGoogle Scholar
Rajchenbach, J., Leroux, A. & Clamond, D. 2011 New standing solitary waves in water. Phys. Rev. Lett. 107, 024502.CrossRefGoogle ScholarPubMed
Rayleigh, L. 1879 On the capillary phenomena of jets. Proc. R. Soc. Lond. 29, 7197.Google Scholar
Riahi, N. 1984 Nonlinear convection in a spherical shell. J. Phys. Soc. Japan 53, 25062512.CrossRefGoogle Scholar
Rucklidge, A. M. & Skeldon, A. C. 2015 Can weakly nonlinear theory explain Faraday wave patterns near onset? J. Fluid Mech. 777, 604632.Google Scholar
Shin, S. 2007 Computation of the curvature field in numerical simulation of multiphase flow. J. Comput. Phys. 222, 872878.CrossRefGoogle Scholar
Shin, S., Chergui, J. & Juric, D. 2017 A solver for massively parallel direct numerical simulation of three-dimensional multiphase flows. J. Mech. Sci. Technol. 31, 17391751.CrossRefGoogle Scholar
Shin, S. & Juric, D. 2007 High order level contour reconstruction method. J. Mech. Sci. Technol. 21, 311326.CrossRefGoogle Scholar
Shin, S. & Juric, D. 2009 A hybrid interface method for three-dimensional multiphase flows based on front-tracking and level set techniques. Intl J. Numer. Meth. Fluids 60, 753778.CrossRefGoogle Scholar
Shu, C. W. & Osher, S. 1989 Efficient implementation of essentially non-oscillatory shock capturing schemes, II. J. Comput. Phys. 83, 3278.CrossRefGoogle Scholar
Silber, M. & Proctor, M. R. E. 1998 Nonlinear competition between small and large hexagonal patterns. Phys. Rev. Lett. 81, 24502453.CrossRefGoogle Scholar
Trinh, E. & Wang, T. G. 1982 Large-amplitude free and driven drop-shape oscillations: experimental observations. J. Fluid Mech. 122, 315338.CrossRefGoogle Scholar
Tryggvason, G., Scardovelli, R. & Zaleski, S. 2011 Direct Numerical Simulation of Gas–Liquid Multiphase Flows. Cambridge University Press.CrossRefGoogle Scholar
Tsamopoulos, J. A. & Brown, R. A. 1983 Nonlinear oscillations of inviscid drops and bubbles. J. Fluid Mech. 127, 514537.CrossRefGoogle Scholar

Ebo-Adou et al. supplementary movie 1

Visualisation of $\ell=1$ mode for spherical drop. The drop is displaced alternately to the left and the right. Length and colors of arrows indicate the velocity of the surrounding air.

Download Ebo-Adou et al. supplementary movie 1(Video)
Video 6 MB

Ebo-Adou et al. supplementary movie 2

Visualisation of $\ell=2$ prolate-oblate pattern of gravitational harmonic waves. Drop interface and velocity field on and outside drop are shown.

Download Ebo-Adou et al. supplementary movie 2(Video)
Video 49 MB

Ebo-Adou et al. supplementary movie 3

Visualisation of $\ell=3$ tetrahedral pattern of capillary subharmonic waves.

Download Ebo-Adou et al. supplementary movie 3(Video)
Video 2 MB

Ebo-Adou et al. supplementary movie 4a

Visualisation of $\ell=4$ cubic-octahedral pattern of capillary subharmonic waves.

Download Ebo-Adou et al. supplementary movie 4a(Video)
Video 1 MB

Ebo-Adou et al. supplementary movie 4b

Visualisation of $\ell=4$ axisymmetric pattern for subharmonic capillary waves. In this stroboscopic film, only snapshots at a single temporal phase are included, emphasizing the overall drift of the pattern

Download Ebo-Adou et al. supplementary movie 4b(Video)
Video 4 MB

Ebo-Adou et al. supplementary movie 5

Visualisation of $\ell=5$ mode for subharmonic capillary waves, showing evolution from axisymmetric to $D_4$ pattern.

Download Ebo-Adou et al. supplementary movie 5(Video)
Video 15 MB

Ebo-Adou et al. supplementary movie 6

Visualisation of $\ell=6$ icosahedral-dodecahedral pattern for subharmonic capillary waves.

Download Ebo-Adou et al. supplementary movie 6(Video)
Video 3 MB